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非对称排斥过程中的动态边界

Dynamic boundaries in asymmetric exclusion processes.

作者信息

Nowak Sarah A, Fok Pak-Wing, Chou Tom

机构信息

Department of Biomathematics, UCLA, Los Angeles, California 90095-1766, USA.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2007 Sep;76(3 Pt 1):031135. doi: 10.1103/PhysRevE.76.031135. Epub 2007 Sep 27.

Abstract

We investigate the dynamics of a one-dimensional asymmetric exclusion process with Langmuir kinetics and a fluctuating wall. At the left-hand boundary, particles are injected onto the lattice; from there, the particles hop to the right. Along the lattice, particles can adsorb or desorb, and the right-hand boundary is defined by a wall particle. The confining wall particle has intrinsic forward and backward hopping, a net leftward drift, and cannot desorb. Performing Monte Carlo simulations and using a moving-frame finite segment approach coupled to mean field theory, we find the parameter regimes in which the wall acquires a steady-state position. In other regimes, the wall will either drift to the left and fall off the lattice at the injection site, or drift indefinitely to the right. Our results are discussed in the context of nonequilibrium phases of the system, fluctuating boundary layers, and particle densities in the laboratory frame versus the frame of the fluctuating wall.

摘要

我们研究了具有朗缪尔动力学和波动壁的一维非对称排斥过程的动力学。在左手边界,粒子被注入到晶格上;从那里开始,粒子向右跳跃。沿着晶格,粒子可以吸附或解吸,右手边界由壁粒子定义。限制壁粒子具有固有的向前和向后跳跃、净向左漂移,并且不能解吸。通过进行蒙特卡罗模拟并使用与平均场理论相结合的移动框架有限段方法,我们找到了壁获得稳态位置的参数区域。在其他区域中,壁要么向左漂移并在注入位点从晶格上脱落,要么无限向右漂移。我们的结果在系统的非平衡相、波动边界层以及实验室坐标系与波动壁坐标系中的粒子密度的背景下进行了讨论。

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